Symmetries of Spatial Graphs and Rational Twists Along Spheres and Tori
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Classification of Finite Abelian Groups
Math 317 C1 John Sullivan Spring 2003 Classification of Finite Abelian Groups (Notes based on an article by Navarro in the Amer. Math. Monthly, February 2003.) The fundamental theorem of finite abelian groups expresses any such group as a product of cyclic groups: Theorem. Suppose G is a finite abelian group. Then G is (in a unique way) a direct product of cyclic groups of order pk with p prime. Our first step will be a special case of Cauchy’s Theorem, which we will prove later for arbitrary groups: whenever p |G| then G has an element of order p. Theorem (Cauchy). If G is a finite group, and p |G| is a prime, then G has an element of order p (or, equivalently, a subgroup of order p). ∼ Proof when G is abelian. First note that if |G| is prime, then G = Zp and we are done. In general, we work by induction. If G has no nontrivial proper subgroups, it must be a prime cyclic group, the case we’ve already handled. So we can suppose there is a nontrivial subgroup H smaller than G. Either p |H| or p |G/H|. In the first case, by induction, H has an element of order p which is also order p in G so we’re done. In the second case, if ∼ g + H has order p in G/H then |g + H| |g|, so hgi = Zkp for some k, and then kg ∈ G has order p. Note that we write our abelian groups additively. Definition. Given a prime p, a p-group is a group in which every element has order pk for some k. -
Crystal Symmetry Groups
X-Ray and Neutron Crystallography rational numbers is a group under Crystal Symmetry Groups multiplication, and both it and the integer group already discussed are examples of infinite groups because they each contain an infinite number of elements. ymmetry plays an important role between the integers obey the rules of In the case of a symmetry group, in crystallography. The ways in group theory: an element is the operation needed to which atoms and molecules are ● There must be defined a procedure for produce one object from another. For arrangeds within a unit cell and unit cells example, a mirror operation takes an combining two elements of the group repeat within a crystal are governed by to form a third. For the integers one object in one location and produces symmetry rules. In ordinary life our can choose the addition operation so another of the opposite hand located first perception of symmetry is what that a + b = c is the operation to be such that the mirror doing the operation is known as mirror symmetry. Our performed and u, b, and c are always is equidistant between them (Fig. 1). bodies have, to a good approximation, elements of the group. These manipulations are usually called mirror symmetry in which our right side ● There exists an element of the group, symmetry operations. They are com- is matched by our left as if a mirror called the identity element and de- bined by applying them to an object se- passed along the central axis of our noted f, that combines with any other bodies. -
1.6 Cyclic Subgroups
1.6. CYCLIC SUBGROUPS 19 1.6 Cyclic Subgroups Recall: cyclic subgroup, cyclic group, generator. Def 1.68. Let G be a group and a ∈ G. If the cyclic subgroup hai is finite, then the order of a is |hai|. Otherwise, a is of infinite order. 1.6.1 Elementary Properties Thm 1.69. Every cyclic group is abelian. Thm 1.70. If m ∈ Z+ and n ∈ Z, then there exist unique q, r ∈ Z such that n = mq + r and 0 ≤ r ≤ m. n In fact, q = b m c and r = n − mq. Here bxc denotes the maximal integer no more than x. Ex 1.71 (Ex 6.4, Ex 6.5, p60). 1. Find the quotient q and the remainder r when n = 38 is divided by m = 7. 2. Find the quotient q and the remainder r when n = −38 is divided by m = 7. Thm 1.72 (Important). A subgroup of a cyclic group is cyclic. Proof. (refer to the book) Ex 1.73. The subgroups of hZ, +i are precisely hnZ, +i for n ∈ Z. Def 1.74. Let r, s ∈ Z. The greatest common divisor (gcd) of r and s is the largest positive integer d that divides both r and s. Written as d = gcd(r, s). In fact, d is the positive generator of the following cyclic subgroup of Z: hdi = {nr + ms | n, m ∈ Z}. So d is the smallest positive integer that can be written as nr + ms for some n, m ∈ Z. Ex 1.75. gcd(36, 63) = 9, gcd(36, 49) = 1. -
And Free Cyclic Group Actions on Homotopy Spheres
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 220, 1976 DECOMPOSABILITYOF HOMOTOPYLENS SPACES ANDFREE CYCLICGROUP ACTIONS ON HOMOTOPYSPHERES BY KAI WANG ABSTRACT. Let p be a linear Zn action on C and let p also denote the induced Z„ action on S2p~l x D2q, D2p x S2q~l and S2p~l x S2q~l " 1m_1 where p = [m/2] and q = m —p. A free differentiable Zn action (£ , ju) on a homotopy sphere is p-decomposable if there is an equivariant diffeomor- phism <t>of (S2p~l x S2q~l, p) such that (S2m_1, ju) is equivalent to (£(*), ¿(*)) where S(*) = S2p_1 x D2q U^, D2p x S2q~l and A(<P) is a uniquely determined action on S(*) such that i4(*)IS p~l XD q = p and A(Q)\D p X S = p. A homotopy lens space is p-decomposable if it is the orbit space of a p-decomposable free Zn action on a homotopy sphere. In this paper, we will study the decomposabilities of homotopy lens spaces. We will also prove that for each lens space L , there exist infinitely many inequivalent free Zn actions on S m such that the orbit spaces are simple homotopy equiva- lent to L 0. Introduction. Let A be the antipodal map and let $ be an equivariant diffeomorphism of (Sp x Sp, A) where A(x, y) = (-x, -y). Then there is a uniquely determined free involution A($) on 2(4>) where 2(4») = Sp x Dp+1 U<¡,Dp+l x Sp such that the inclusions S" x Dp+l —+ 2(d>), Dp+1 x Sp —*■2(4>) are equi- variant. -
Molecular Symmetry
Molecular Symmetry 1 I. WHAT IS SYMMETRY AND WHY IT IS IMPORTANT? Some object are ”more symmetrical” than others. A sphere is more symmetrical than a cube because it looks the same after rotation through any angle about the diameter. A cube looks the same only if it is rotated through certain angels about specific axes, such as 90o, 180o, or 270o about an axis passing through the centers of any of its opposite faces, or by 120o or 240o about an axis passing through any of the opposite corners. Here are also examples of different molecules which remain the same after certain symme- try operations: NH3, H2O, C6H6, CBrClF . In general, an action which leaves the object looking the same after a transformation is called a symmetry operation. Typical symme- try operations include rotations, reflections, and inversions. There is a corresponding symmetry element for each symmetry operation, which is the point, line, or plane with respect to which the symmetry operation is performed. For instance, a rotation is carried out around an axis, a reflection is carried out in a plane, while an inversion is carried our in a point. We shall see that we can classify molecules that possess the same set of symmetry ele- ments, and grouping together molecules that possess the same set of symmetry elements. This classification is very important, because it allows to make some general conclusions about molecular properties without calculation. Particularly, we will be able to decide if a molecule has a dipole moment, or not and to know in advance the degeneracy of molecular states. -
A STUDY on the ALGEBRAIC STRUCTURE of SL 2(Zpz)
A STUDY ON THE ALGEBRAIC STRUCTURE OF SL2 Z pZ ( ~ ) A Thesis Presented to The Honors Tutorial College Ohio University In Partial Fulfillment of the Requirements for Graduation from the Honors Tutorial College with the degree of Bachelor of Science in Mathematics by Evan North April 2015 Contents 1 Introduction 1 2 Background 5 2.1 Group Theory . 5 2.2 Linear Algebra . 14 2.3 Matrix Group SL2 R Over a Ring . 22 ( ) 3 Conjugacy Classes of Matrix Groups 26 3.1 Order of the Matrix Groups . 26 3.2 Conjugacy Classes of GL2 Fp ....................... 28 3.2.1 Linear Case . .( . .) . 29 3.2.2 First Quadratic Case . 29 3.2.3 Second Quadratic Case . 30 3.2.4 Third Quadratic Case . 31 3.2.5 Classes in SL2 Fp ......................... 33 3.3 Splitting of Classes of(SL)2 Fp ....................... 35 3.4 Results of SL2 Fp ..............................( ) 40 ( ) 2 4 Toward Lifting to SL2 Z p Z 41 4.1 Reduction mod p ...............................( ~ ) 42 4.2 Exploring the Kernel . 43 i 4.3 Generalizing to SL2 Z p Z ........................ 46 ( ~ ) 5 Closing Remarks 48 5.1 Future Work . 48 5.2 Conclusion . 48 1 Introduction Symmetries are one of the most widely-known examples of pure mathematics. Symmetry is when an object can be rotated, flipped, or otherwise transformed in such a way that its appearance remains the same. Basic geometric figures should create familiar examples, take for instance the triangle. Figure 1: The symmetries of a triangle: 3 reflections, 2 rotations. The red lines represent the reflection symmetries, where the trianlge is flipped over, while the arrows represent the rotational symmetry of the triangle. -
Order (Group Theory) 1 Order (Group Theory)
Order (group theory) 1 Order (group theory) In group theory, a branch of mathematics, the term order is used in two closely-related senses: • The order of a group is its cardinality, i.e., the number of its elements. • The order, sometimes period, of an element a of a group is the smallest positive integer m such that am = e (where e denotes the identity element of the group, and am denotes the product of m copies of a). If no such m exists, a is said to have infinite order. All elements of finite groups have finite order. The order of a group G is denoted by ord(G) or |G| and the order of an element a by ord(a) or |a|. Example Example. The symmetric group S has the following multiplication table. 3 • e s t u v w e e s t u v w s s e v w t u t t u e s w v u u t w v e s v v w s e u t w w v u t s e This group has six elements, so ord(S ) = 6. By definition, the order of the identity, e, is 1. Each of s, t, and w 3 squares to e, so these group elements have order 2. Completing the enumeration, both u and v have order 3, for u2 = v and u3 = vu = e, and v2 = u and v3 = uv = e. Order and structure The order of a group and that of an element tend to speak about the structure of the group. -
Special Unitary Group - Wikipedia
Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Special unitary group In mathematics, the special unitary group of degree n, denoted SU( n), is the Lie group of n×n unitary matrices with determinant 1. (More general unitary matrices may have complex determinants with absolute value 1, rather than real 1 in the special case.) The group operation is matrix multiplication. The special unitary group is a subgroup of the unitary group U( n), consisting of all n×n unitary matrices. As a compact classical group, U( n) is the group that preserves the standard inner product on Cn.[nb 1] It is itself a subgroup of the general linear group, SU( n) ⊂ U( n) ⊂ GL( n, C). The SU( n) groups find wide application in the Standard Model of particle physics, especially SU(2) in the electroweak interaction and SU(3) in quantum chromodynamics.[1] The simplest case, SU(1) , is the trivial group, having only a single element. The group SU(2) is isomorphic to the group of quaternions of norm 1, and is thus diffeomorphic to the 3-sphere. Since unit quaternions can be used to represent rotations in 3-dimensional space (up to sign), there is a surjective homomorphism from SU(2) to the rotation group SO(3) whose kernel is {+ I, − I}. [nb 2] SU(2) is also identical to one of the symmetry groups of spinors, Spin(3), that enables a spinor presentation of rotations. Contents Properties Lie algebra Fundamental representation Adjoint representation The group SU(2) Diffeomorphism with S 3 Isomorphism with unit quaternions Lie Algebra The group SU(3) Topology Representation theory Lie algebra Lie algebra structure Generalized special unitary group Example Important subgroups See also 1 of 10 2/22/2018, 8:54 PM Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Remarks Notes References Properties The special unitary group SU( n) is a real Lie group (though not a complex Lie group). -
Chapter 1 Group and Symmetry
Chapter 1 Group and Symmetry 1.1 Introduction 1. A group (G) is a collection of elements that can ‘multiply’ and ‘di- vide’. The ‘multiplication’ ∗ is a binary operation that is associative but not necessarily commutative. Formally, the defining properties are: (a) if g1, g2 ∈ G, then g1 ∗ g2 ∈ G; (b) there is an identity e ∈ G so that g ∗ e = e ∗ g = g for every g ∈ G. The identity e is sometimes written as 1 or 1; (c) there is a unique inverse g−1 for every g ∈ G so that g ∗ g−1 = g−1 ∗ g = e. The multiplication rules of a group can be listed in a multiplication table, in which every group element occurs once and only once in every row and every column (prove this !) . For example, the following is the multiplication table of a group with four elements named Z4. e g1 g2 g3 e e g1 g2 g3 g1 g1 g2 g3 e g2 g2 g3 e g1 g3 g3 e g1 g2 Table 2.1 Multiplication table of Z4 3 4 CHAPTER 1. GROUP AND SYMMETRY 2. Two groups with identical multiplication tables are usually considered to be the same. We also say that these two groups are isomorphic. Group elements could be familiar mathematical objects, such as numbers, matrices, and differential operators. In that case group multiplication is usually the ordinary multiplication, but it could also be ordinary addition. In the latter case the inverse of g is simply −g, the identity e is simply 0, and the group multiplication is commutative. -
Finite Abelian P-Primary Groups
CLASSIFICATION OF FINITE ABELIAN GROUPS 1. The main theorem Theorem 1.1. Let A be a finite abelian group. There is a sequence of prime numbers p p p 1 2 ··· n (not necessarily all distinct) and a sequence of positive integers a1,a2,...,an such that A is isomorphic to the direct product ⇠ a1 a2 an A Zp Zp Zpn . ! 1 ⇥ 2 ⇥···⇥ In particular n A = pai . | | i iY=n Example 1.2. We can classify abelian groups of order 144 = 24 32. Here are the possibilities, with the partitions of the powers of 2 and 3 on⇥ the right: Z2 Z2 Z2 Z2 Z3 Z3;(4, 2) = (1 + 1 + 1 + 1, 1 + 1) ⇥ ⇥ ⇥ ⇥ ⇥ Z2 Z2 Z4 Z3 Z3;(4, 2) = (1 + 1 + 2, 1 + 1) ⇥ ⇥ ⇥ ⇥ Z4 Z4 Z3 Z3;(4, 2) = (2 + 2, 1 + 1) ⇥ ⇥ ⇥ Z2 Z8 Z3 Z3;(4, 2) = (1 + 3, 1 + 1) ⇥ ⇥ ⇥ Z16 Z3 Z3;(4, 2) = (4, 1 + 1) ⇥ ⇥ Z2 Z2 Z2 Z2 Z9;(4, 2) = (1 + 1 + 1 + 1, 2) ⇥ ⇥ ⇥ ⇥ Z2 Z2 Z4 Z9;(4, 2) = (1 + 1 + 2, 2) ⇥ ⇥ ⇥ Z4 Z4 Z9;(4, 2) = (2 + 2, 2) ⇥ ⇥ Z2 Z8 Z9;(4, 2) = (1 + 3, 2) ⇥ ⇥ Z16 Z9 cyclic, isomorphic to Z144;(4, 2) = (4, 2). ⇥ There are 10 non-isomorphic abelian groups of order 144. Theorem 1.1 can be broken down into two theorems. 1 2CLASSIFICATIONOFFINITEABELIANGROUPS Theorem 1.3. Let A be a finite abelian group. Let q1,...,qr be the distinct primes dividing A ,andsay | | A = qbj . | | j Yj Then there are subgroups A A, j =1,...,r,with A = qbj ,andan j ✓ | j| j isomorphism A ⇠ A A A . -
MATH 433 Applied Algebra Lecture 19: Subgroups (Continued). Error-Detecting and Error-Correcting Codes. Subgroups Definition
MATH 433 Applied Algebra Lecture 19: Subgroups (continued). Error-detecting and error-correcting codes. Subgroups Definition. A group H is a called a subgroup of a group G if H is a subset of G and the group operation on H is obtained by restricting the group operation on G. Let S be a nonempty subset of a group G. The group generated by S, denoted hSi, is the smallest subgroup of G that contains the set S. The elements of the set S are called generators of the group hSi. Theorem (i) The group hSi is the intersection of all subgroups of G that contain the set S. (ii) The group hSi consists of all elements of the form g1g2 . gk , where each gi is either a generator s ∈ S or the inverse s−1 of a generator. A cyclic group is a subgroup generated by a single element: hgi = {g n : n ∈ Z}. Lagrange’s theorem The number of elements in a group G is called the order of G and denoted o(G). Given a subgroup H of G, the number of cosets of H in G is called the index of H in G and denoted [G : H]. Theorem (Lagrange) If H is a subgroup of a finite group G, then o(G) = [G : H] · o(H). In particular, the order of H divides the order of G. Corollary (i) If G is a finite group, then the order of any element g ∈ G divides the order of G. (ii) If G is a finite group, then g o(G) = 1 for all g ∈ G. -
Arxiv:1305.5974V1 [Math-Ph]
INTRODUCTION TO SPORADIC GROUPS for physicists Luis J. Boya∗ Departamento de F´ısica Te´orica Universidad de Zaragoza E-50009 Zaragoza, SPAIN MSC: 20D08, 20D05, 11F22 PACS numbers: 02.20.a, 02.20.Bb, 11.24.Yb Key words: Finite simple groups, sporadic groups, the Monster group. Juan SANCHO GUIMERA´ In Memoriam Abstract We describe the collection of finite simple groups, with a view on physical applications. We recall first the prime cyclic groups Zp, and the alternating groups Altn>4. After a quick revision of finite fields Fq, q = pf , with p prime, we consider the 16 families of finite simple groups of Lie type. There are also 26 extra “sporadic” groups, which gather in three interconnected “generations” (with 5+7+8 groups) plus the Pariah groups (6). We point out a couple of physical applications, in- cluding constructing the biggest sporadic group, the “Monster” group, with close to 1054 elements from arguments of physics, and also the relation of some Mathieu groups with compactification in string and M-theory. ∗[email protected] arXiv:1305.5974v1 [math-ph] 25 May 2013 1 Contents 1 Introduction 3 1.1 Generaldescriptionofthework . 3 1.2 Initialmathematics............................ 7 2 Generalities about groups 14 2.1 Elementarynotions............................ 14 2.2 Theframeworkorbox .......................... 16 2.3 Subgroups................................. 18 2.4 Morphisms ................................ 22 2.5 Extensions................................. 23 2.6 Familiesoffinitegroups ......................... 24 2.7 Abeliangroups .............................. 27 2.8 Symmetricgroup ............................. 28 3 More advanced group theory 30 3.1 Groupsoperationginspaces. 30 3.2 Representations.............................. 32 3.3 Characters.Fourierseries . 35 3.4 Homological algebra and extension theory . 37 3.5 Groupsuptoorder16..........................